Jump to
S1C2
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -79.336058 |
| Energy at 298.15K | -79.342000 |
| HF Energy | -79.336058 |
| Nuclear repulsion energy | 42.147915 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B1B95/3-21G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1g |
3078 |
2944 |
0.00 |
185.10 |
0.01 |
0.02 |
| 2 |
A1g |
1463 |
1399 |
0.00 |
9.40 |
0.72 |
0.84 |
| 3 |
A1g |
999 |
956 |
0.00 |
8.00 |
0.29 |
0.45 |
| 4 |
A1u |
309 |
295 |
0.00 |
0.00 |
0.00 |
0.00 |
| 5 |
A2u |
3078 |
2945 |
43.73 |
0.00 |
0.00 |
0.00 |
| 6 |
A2u |
1470 |
1406 |
9.77 |
0.00 |
0.00 |
0.00 |
| 7 |
Eg |
3135 |
2999 |
0.00 |
119.03 |
0.75 |
0.86 |
| 7 |
Eg |
3135 |
2999 |
0.00 |
119.04 |
0.75 |
0.86 |
| 8 |
Eg |
1573 |
1505 |
0.00 |
46.03 |
0.75 |
0.86 |
| 8 |
Eg |
1573 |
1505 |
0.00 |
46.03 |
0.75 |
0.86 |
| 9 |
Eg |
1258 |
1203 |
0.00 |
3.57 |
0.75 |
0.86 |
| 9 |
Eg |
1258 |
1203 |
0.00 |
3.57 |
0.75 |
0.86 |
| 10 |
Eu |
3162 |
3025 |
51.55 |
0.00 |
0.00 |
0.00 |
| 10 |
Eu |
3162 |
3025 |
51.55 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1573 |
1505 |
14.03 |
0.00 |
0.00 |
0.00 |
| 11 |
Eu |
1573 |
1505 |
14.03 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
864 |
827 |
9.96 |
0.00 |
0.00 |
0.00 |
| 12 |
Eu |
864 |
827 |
9.96 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 16762.5 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 16036.6 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B1B95/3-21G
Point Group is D3d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.768 |
| C2 |
0.000 |
0.000 |
-0.768 |
| H3 |
0.000 |
1.021 |
1.157 |
| H4 |
-0.884 |
-0.511 |
1.157 |
| H5 |
0.884 |
-0.511 |
1.157 |
| H6 |
0.000 |
-1.021 |
-1.157 |
| H7 |
-0.884 |
0.511 |
-1.157 |
| H8 |
0.884 |
0.511 |
-1.157 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5352 | 1.0929 | 1.0929 | 1.0929 | 2.1789 | 2.1789 | 2.1789 |
C2 | 1.5352 | | 2.1789 | 2.1789 | 2.1789 | 1.0929 | 1.0929 | 1.0929 | H3 | 1.0929 | 2.1789 | | 1.7686 | 1.7686 | 3.0866 | 2.5296 | 2.5296 | H4 | 1.0929 | 2.1789 | 1.7686 | | 1.7686 | 2.5296 | 2.5296 | 3.0866 | H5 | 1.0929 | 2.1789 | 1.7686 | 1.7686 | | 2.5296 | 3.0866 | 2.5296 | H6 | 2.1789 | 1.0929 | 3.0866 | 2.5296 | 2.5296 | | 1.7686 | 1.7686 | H7 | 2.1789 | 1.0929 | 2.5296 | 2.5296 | 3.0866 | 1.7686 | | 1.7686 | H8 | 2.1789 | 1.0929 | 2.5296 | 3.0866 | 2.5296 | 1.7686 | 1.7686 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
110.881 |
|
C1 |
C2 |
H7 |
110.881 |
| C1 |
C2 |
H8 |
110.881 |
|
C2 |
C1 |
H3 |
110.881 |
| C2 |
C1 |
H4 |
110.881 |
|
C2 |
C1 |
H5 |
110.881 |
| H3 |
C1 |
H4 |
108.025 |
|
H3 |
C1 |
H5 |
108.025 |
| H4 |
C1 |
H5 |
108.025 |
|
H6 |
C2 |
H7 |
108.025 |
| H6 |
C2 |
H8 |
108.025 |
|
H7 |
C2 |
H8 |
108.025 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.620 |
|
|
|
| 2 |
C |
-0.620 |
|
|
|
| 3 |
H |
0.207 |
|
|
|
| 4 |
H |
0.207 |
|
|
|
| 5 |
H |
0.207 |
|
|
|
| 6 |
H |
0.207 |
|
|
|
| 7 |
H |
0.207 |
|
|
|
| 8 |
H |
0.207 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.682 |
0.000 |
0.000 |
| y |
0.000 |
-14.682 |
0.000 |
| z |
0.000 |
0.000 |
-15.078 |
|
| Traceless |
| | x | y | z |
| x |
0.198 |
0.000 |
0.000 |
| y |
0.000 |
0.198 |
0.000 |
| z |
0.000 |
0.000 |
-0.396 |
|
| Polar |
| 3z2-r2 | -0.792 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.120 |
0.000 |
0.000 |
| y |
0.000 |
3.120 |
0.000 |
| z |
0.000 |
0.000 |
3.332 |
<r2> (average value of r
2) Å
2
| <r2> |
30.613 |
| (<r2>)1/2 |
5.533 |
Jump to
S1C1
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -79.331711 |
| Energy at 298.15K | |
| HF Energy | -79.331711 |
| Nuclear repulsion energy | 41.985212 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B1B95/3-21G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1' |
3095 |
2961 |
0.00 |
|
|
|
| 2 |
A1' |
1489 |
1424 |
0.00 |
|
|
|
| 3 |
A1' |
990 |
947 |
0.00 |
|
|
|
| 4 |
A1" |
296i |
283i |
0.00 |
|
|
|
| 5 |
A2" |
3088 |
2955 |
45.98 |
|
|
|
| 6 |
A2" |
1468 |
1405 |
9.70 |
|
|
|
| 7 |
E' |
3171 |
3033 |
43.21 |
|
|
|
| 7 |
E' |
3171 |
3033 |
43.21 |
|
|
|
| 8 |
E' |
1585 |
1516 |
16.01 |
|
|
|
| 8 |
E' |
1585 |
1516 |
16.00 |
|
|
|
| 9 |
E' |
942 |
902 |
9.80 |
|
|
|
| 9 |
E' |
942 |
902 |
9.80 |
|
|
|
| 10 |
E" |
3148 |
3012 |
0.00 |
|
|
|
| 10 |
E" |
3148 |
3012 |
0.00 |
|
|
|
| 11 |
E" |
1573 |
1505 |
0.00 |
|
|
|
| 11 |
E" |
1573 |
1505 |
0.00 |
|
|
|
| 12 |
E" |
1212 |
1159 |
0.00 |
|
|
|
| 12 |
E" |
1212 |
1159 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16547.3 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 15830.8 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B1B95/3-21G
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.774 |
| C2 |
0.000 |
0.000 |
-0.774 |
| H3 |
0.000 |
1.017 |
1.171 |
| H4 |
-0.881 |
-0.509 |
1.171 |
| H5 |
0.881 |
-0.509 |
1.171 |
| H6 |
0.000 |
1.017 |
-1.171 |
| H7 |
0.881 |
-0.509 |
-1.171 |
| H8 |
-0.881 |
-0.509 |
-1.171 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5490 | 1.0919 | 1.0919 | 1.0919 | 2.1957 | 2.1957 | 2.1957 |
C2 | 1.5490 | | 2.1957 | 2.1957 | 2.1957 | 1.0919 | 1.0919 | 1.0919 | H3 | 1.0919 | 2.1957 | | 1.7618 | 1.7618 | 2.3428 | 2.9314 | 2.9314 | H4 | 1.0919 | 2.1957 | 1.7618 | | 1.7618 | 2.9314 | 2.9314 | 2.3428 | H5 | 1.0919 | 2.1957 | 1.7618 | 1.7618 | | 2.9314 | 2.3428 | 2.9314 | H6 | 2.1957 | 1.0919 | 2.3428 | 2.9314 | 2.9314 | | 1.7618 | 1.7618 | H7 | 2.1957 | 1.0919 | 2.9314 | 2.9314 | 2.3428 | 1.7618 | | 1.7618 | H8 | 2.1957 | 1.0919 | 2.9314 | 2.3428 | 2.9314 | 1.7618 | 1.7618 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
H6 |
111.318 |
|
C1 |
C2 |
H7 |
111.318 |
| C1 |
C2 |
H8 |
111.318 |
|
C2 |
C1 |
H3 |
111.318 |
| C2 |
C1 |
H4 |
111.318 |
|
C2 |
C1 |
H5 |
111.318 |
| H3 |
C1 |
H4 |
107.563 |
|
H3 |
C1 |
H5 |
107.563 |
| H4 |
C1 |
H5 |
107.563 |
|
H6 |
C2 |
H7 |
107.563 |
| H6 |
C2 |
H8 |
107.563 |
|
H7 |
C2 |
H8 |
107.563 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.629 |
|
|
|
| 2 |
C |
-0.629 |
|
|
|
| 3 |
H |
0.210 |
|
|
|
| 4 |
H |
0.210 |
|
|
|
| 5 |
H |
0.210 |
|
|
|
| 6 |
H |
0.210 |
|
|
|
| 7 |
H |
0.210 |
|
|
|
| 8 |
H |
0.210 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.667 |
0.000 |
0.000 |
| y |
0.000 |
-14.667 |
0.000 |
| z |
0.000 |
0.000 |
-14.975 |
|
| Traceless |
| | x | y | z |
| x |
0.154 |
0.000 |
0.000 |
| y |
0.000 |
0.154 |
0.000 |
| z |
0.000 |
0.000 |
-0.308 |
|
| Polar |
| 3z2-r2 | -0.615 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.051 |
0.000 |
0.000 |
| y |
0.000 |
3.051 |
0.000 |
| z |
0.000 |
0.000 |
3.284 |
<r2> (average value of r
2) Å
2
| <r2> |
30.864 |
| (<r2>)1/2 |
5.556 |